Spin-Momentum Correlations, Aharonov-Bohm, and Color Entanglement in Quantum Chromodynamics

Transcription

1 Spin-Momentum Correlations, Aharonov-Bohm, and Color Entanglement in Quantum Chromodynamics Christine A. Aidala University of Michigan left right CENPA Seminar University of Washington February 1, 2018

2 Theory of strong nuclear interaction: Quantum Chromodynamics Fundamental field theory in hand since the early 1970s BUT... Quark and gluon degrees of freedom in the theory cannot be observed or manipulated directly in experiment! Color confinement quarks and gluons are confined to color-neutral bound states CLAS, PRL 113, (2014) PRL Editor s Choice Oct Christine Aidala, CENPA Seminar, 2/1/18 2

3 How do we understand the visible matter in our universe in terms of the quark and gluon degrees of freedom of quantum chromodynamics? How can studying QCD systems teach us more about fundamental aspects of QCD as a theory? Christine Aidala, CENPA Seminar, 2/1/18 3

4 The proton as a laboratory for Proton: simplest stable QCD bound state studying QCD Different energy scales offer information on different aspects of proton internal structure Josh Rubin Christine Aidala, CENPA Seminar, 2/1/18 4

5 Quark distribution functions inside the proton: The language we ve developed (so far!) What momentum fraction would the scattering particle carry if the proton were made of A point-like particle 3 bound valence quarks 3 valence quarks momentum fraction 1 3 bound valence quarks + some low-momentum sea quarks 1/3 1 momentum fraction Sea Valence 1/3 momentum fraction Halzen and Martin, Quarks and Leptons, p Christine Aidala, CENPA Seminar, 2/1/18 small momentum 1/3 momentum fraction 5 1

6 Quark distribution functions inside the proton: The language we ve developed (so far!) What momentum fraction would the scattering particle carry if the proton were made of A point-like particle 3 bound valence quarks 3 valence quarks momentum fraction 1 3 bound valence quarks + some low-momentum sea quarks 1/3 1 momentum fraction Sea Valence 1/3 momentum fraction Halzen and Martin, Quarks and Leptons, p Christine Aidala, CENPA Seminar, 2/1/18 small momentum 1/3 momentum fraction 5 1

7 Quark distribution functions inside the proton: The language we ve developed (so far!) What momentum fraction would the scattering particle carry if the proton were made of A point-like particle 3 bound valence quarks 3 valence quarks momentum fraction 1 3 bound valence quarks + some low-momentum sea quarks 1/3 1 momentum fraction Sea Valence 1/3 momentum fraction Halzen and Martin, Quarks and Leptons, p Christine Aidala, CENPA Seminar, 2/1/18 small momentum 1/3 momentum fraction 5 1

8 Quark distribution functions inside the proton: The language we ve developed (so far!) What momentum fraction would the scattering particle carry if the proton were made of A point-like particle 3 bound valence quarks 3 valence quarks momentum fraction 1 3 bound valence quarks + some low-momentum sea quarks 1/3 1 momentum fraction Sea Valence 1/3 momentum fraction Halzen and Martin, Quarks and Leptons, p Christine Aidala, CENPA Seminar, 2/1/18 small momentum 1/3 momentum fraction 5 1

9 What have we learned in terms of this picture by now? Up and down quark valence distributions peaked ~1/3 Lots of sea quarkantiquark pairs and even more gluons! distribution function PRD67, momentum fraction (2003) Christine Aidala, CENPA Seminar, 2/1/18 6

10 What have we learned in terms of this picture by now? Up and down quark valence distributions peaked ~1/3 Lots of sea quarkantiquark pairs and even more gluons! parton distribution function PRD67, momentum fraction (2003) Christine Aidala, CENPA Seminar, 2/1/18 6

11 Perturbative QCD Take advantage of running of strong coupling constant with energy (asymptotic freedom) weak coupling at high energies (short distances) Perturbative expansion as in quantum electrodynamics (but many more diagrams due to gluon self-coupling!!) Christine Aidala, CENPA Seminar, 2/1/18 7

12 Perturbative QCD Take advantage of running of strong coupling constant with energy (asymptotic freedom) weak coupling at high energies (short distances) Perturbative expansion as in quantum electrodynamics (but many more diagrams due to gluon self-coupling!!) Provides one rigorous way of relating the fundamental field theory to a variety of physical Christine Aidala, CENPA observables! Seminar, 2/1/18 7

13 Factorization and universality in perturbative QCD Systematically factorize short- and long-distance physics Observable physical QCD processes always involve at least one long-distance scale of ~10-15 m describing boundstate structure (confinement)! Long-distance (i.e. not perturbatively calculable) functions describing structure need to be universal Physically meaningful descriptions Portable across calculations for many processes Constrain functions describing proton structure by measuring scattering cross sections in many colliding systems over wide kinematic range and performing simultaneous fits to world data Christine Aidala, CENPA Seminar, 2/1/18 8

14 Factorization and universality in perturbative QCD Systematically factorize short- and long-distance physics Observable physical QCD processes always involve at least one long-distance scale of ~10-15 m describing boundstate structure (confinement)! Note: Nonperturbative lattice Long-distance (i.e. not perturbatively QCD calculable) techniques have made functions describing structure need tremendous to be universal progress toward ab Physically meaningful descriptions initio calculations of proton Portable across calculations for many processes structure in last ~5 years! Constrain functions describing proton structure by measuring scattering cross sections in many colliding systems over wide kinematic range and performing simultaneous fits to world data Christine Aidala, CENPA Seminar, 2/1/18 8

15 Mapping out the quark-gluon structure of the proton What does the proton look like in terms of the quarks and gluons inside it? Position Momentum Spin Flavor Color Vast majority of past four decades focused on 1-dimensional momentum structure! Since 1990s starting to consider transverse components... Christine Aidala, CENPA Seminar, 2/1/18 9

16 Mapping out the quark-gluon structure of the proton What does the proton look like in terms of the quarks and gluons inside it? Position Momentum Spin Flavor Color Polarized protons first studied in 1980s. How angular momentum of quarks and gluons add up still not well understood! Christine Aidala, CENPA Seminar, 2/1/18 9

17 Mapping out the quark-gluon structure of the proton What does the proton look like in terms of the quarks and gluons inside it? Position Momentum Spin Flavor Color Good measurements of flavor distributions in valence region. Flavor structure at lower momentum fractions still yielding surprises! Christine Aidala, CENPA Seminar, 2/1/18 9

18 Mapping out the quark-gluon structure of the proton What does the proton look like in terms of the quarks and gluons inside it? Position Momentum Spin Flavor Color Theoretical and experimental concepts to describe and access position only born in mid-1990s. Pioneering measurements over past decade. Christine Aidala, CENPA Seminar, 2/1/18 9

19 Mapping out the quark-gluon structure of the proton What does the proton look like in terms of the quarks and gluons inside it? Position Momentum Spin Flavor Color Accounted for theoretically from beginning of QCD, but more detailed, potentially observable effects of color flow have come to forefront in last few years... Christine Aidala, CENPA Seminar, 2/1/18 9

20 Spin-momentum correlations: 1976 discovery in p+p collisions Argonne s=4.9 GeV Charged pions produced preferentially on one or the other side with respect to the transversely polarized beam direction by up to 40%!! pp πx Had to wait more than a decade for the birth of a new subfield in order to explore the possibilities... left right W.H. Dragoset et al., PRL36, 929 (1976) x = 2 p F long / s Christine Aidala, CENPA Seminar, 2/1/18 10

21 Transverse-momentum-dependent distributions and single-spin asymmetries 1990: D.W. Sivers departs from traditional collinear factorization assumption in pqcd and proposes correlation between the intrinsic transverse motion of the quarks and gluons and the proton s spin D.W. Sivers PRD41, 83 (1990) s ( p 1 p2) Christine Aidala, CENPA Seminar, 2/1/18 Spin and momenta of quarks and/or bound states 11

22 Transverse-momentum-dependent distributions and single-spin asymmetries 1990: D.W. Sivers departs from traditional collinear factorization assumption in pqcd and proposes correlation between the intrinsic transverse motion of the quarks and gluons and the proton s spin First quark distribution function describing a spin-momentum correlation in the proton D.W. Sivers PRD41, 83 (1990) s ( p 1 p2) Christine Aidala, CENPA Seminar, 2/1/18 Spin and momenta of quarks and/or bound states 11

23 Transverse-momentum-dependent distributions and single-spin asymmetries 1990: D.W. Sivers departs from traditional collinear factorization assumption in pqcd and proposes correlation between the intrinsic transverse motion of the quarks and gluons and the proton s spin First quark distribution function describing a spin-momentum correlation in the proton New frontier! Quark dynamics inside QCD bound states, and in their formation process D.W. Sivers PRD41, 83 (1990) s ( p 1 p2) Christine Aidala, CENPA Seminar, 2/1/18 Spin and momenta of quarks and/or bound states 11

24 Spin-spin and spin-momentum correlations in QCD bound states Unpolarized Spin-spin correlations Spin-momentum correlations Christine Aidala, CENPA Seminar, 2/1/18 12

25 Spin-spin and spin-momentum correlations in QCD bound states Unpolarized Worm-gear (Kotzinian-Mulders) Spin-spin correlations Helicity Transversity Spin-momentum correlations Sivers Boer-Mulders Worm-gear Pretzelosity Christine Aidala, CENPA Seminar, 2/1/18 12

26 Spin-spin and spin-momentum correlations in QCD bound states Unpolarized Worm-gear (Kotzinian-Mulders) Spin-spin correlations Helicity Transversity G.A. Miller, Phys. Rev. C68, (2003) Spin-momentum correlations Sivers Boer-Mulders Worm-gear Pretzelosity Christine Aidala, CENPA Seminar, 2/1/18 12

27 Spin-spin and spin-momentum correlations in QCD bound states Unpolarized Worm-gear (Kotzinian-Mulders) Spin-spin correlations Helicity Lots of evidence from deep-inelastic Transversity lepton-nucleon scattering experiments over past ~12 years that many of these correlations are nonzero in nature! Spin-momentum correlations Sivers Boer-Mulders Worm-gear Pretzelosity Christine Aidala, CENPA Seminar, 2/1/18 12

28 Sivers e+p µ+p e+p Boer-Mulders x Collins HERMES, PRD 87, (2013) e+p µ+p Transversity x Collins Christine Aidala, CENPA Seminar, 2/1/18 13

29 Sivers e+p µ+p BELLE PRL96, (2006) Collins x Collins e + e - e+p Boer-Mulders x Collins HERMES, PRD 87, (2013) e+p µ+p Transversity x Collins Christine Aidala, CENPA Seminar, 2/1/18 13

30 But what about proton-proton collisions? ANL s=4.9 GeV BNL s=6.6 GeV FNAL s=19.4 GeV RHIC s=62.4 GeV Aidala, Bass, Hasch, Mallot, RMP 85, 655 (2013) xf = 2 plong / s left Christine Aidala, CENPA Seminar, 2/1/18 right 14

31 But what about proton-proton collisions? ANL s=4.9 GeV BNL s=6.6 GeV FNAL s=19.4 GeV RHIC s=62.4 GeV Aidala, Bass, Hasch, Mallot, RMP 85, 655 (2013) left Much larger spin-momentum correlations, and strikingly similar xf = 2 plong / s effects across energies! Christine Aidala, CENPA Seminar, 2/1/18 right 14

32 Single-spin asymmetries in transversely polarized proton-proton collisions A N A N x F = 0.6 STAR π 0 Effects persist to kinematic regimes where perturbative QCD techniques clearly apply left p T GeV/c right Christine Aidala, CENPA Seminar, 2/1/18 15

33 proton-proton pion + X: Challenging to interpret Always huge effects! But in p+p pion +X don t have enough information to separate initial-state (proton structure) from final-state (pion formation) effects Need to think more carefully... Christine Aidala, CENPA Seminar, 2/1/18 16

34 Different symmetry properties for different spin-momentum correlations Some transverse-momentum-dependent parton distribution functions odd under a parity- and time-reversal (PT) transformation In 1993, after original 1990 paper by D.W. Sivers, J.C. Collins claimed such functions must vanish Only realized in 2002 by Brodsky, Hwang, and Schmidt that could be nonvanishing if phase interference effects due to color interactions present Christine Aidala, CENPA Seminar, 2/1/18 17

35 Different symmetry properties for different spin-momentum correlations Some transverse-momentum-dependent parton distribution functions odd under a parity- and time-reversal (PT) transformation In 1993, after original 1990 paper by D.W. Sivers, J.C. Collins claimed such functions must vanish Only realized in 2002 by Brodsky, Hwang, and Schmidt that could be nonvanishing if phase interference effects due to color interactions present Christine Aidala, CENPA Seminar, 2/1/18 17

36 Different symmetry properties for different spin-momentum correlations Some transverse-momentum-dependent parton distribution functions odd under a parity- and time-reversal (PT) transformation In 1993, after original 1990 paper by D.W. Sivers, J.C. Collins claimed such functions must vanish Only realized in 2002 by Brodsky, Hwang, and Schmidt that could be nonvanishing if phase interference effects due to color interactions present Christine Aidala, CENPA Seminar, 2/1/18 17

37 Modified universality of PT-odd correlations: Color in action! Deep-inelastic lepton-nucleon scattering: Final-state color exchange incoming electron scattering quark scattered electron scattered quark Quark-antiquark annihilation to leptons: Initial-state color exchange incoming proton scattering antiquark scattering quark proton remnant produced positron incoming proton proton remnant incoming proton Christine Aidala, CENPA Seminar, 2/1/18 proton remnant Figures by J.D. Osborn produced electron Opposite sign for PT-odd transverse-momentum-dependent distributions measured in these two processes: process-dependent! (Collins 2002) 18

38 Modified universality: Initial experimental hints Predictions including sign change } STAR PRL 116, (2016) PRL 119, (2017) First measurements by STAR at RHIC and COMPASS at CERN suggestive of predicted sign change in color-annihilation processes compared to quark knock-out by an electron. More statistics forthcoming... Christine Aidala, CENPA Seminar, 2/1/18 19

39 Modified universality requires full QCD: Gauge-invariant quantum field theory From 1993 claim by J.C. Collins that such processes must vanish Slide from M. Anselmino, Transversity 2014 Christine Aidala, CENPA Seminar, 2/1/18 20

40 Physical consequences of a gauge-invariant quantum theory: Aharonov-Bohm (1959) Wikipedia: The Aharonov Bohm effect is important conceptually because it bears on three issues apparent in the recasting of (Maxwell's) classical electromagnetic theory as a gauge theory, which before the advent of quantum mechanics could be argued to be a mathematical reformulation with no physical consequences. The Aharonov Bohm thought experiments and their experimental realization imply that the issues were not just philosophical. The three issues are: whether potentials are "physical" or just a convenient tool for calculating force fields; whether action principles are fundamental; the principle of locality. Christine Aidala, CENPA Seminar, 2/1/18 21

41 Physical consequences of a gauge-invariant quantum theory: Aharonov-Bohm (1959) Physics Today, September 2009 : The Aharonov Bohm effects: Variations on a subtle theme, by Herman Batelaan and Akira Tonomura. Aharonov stresses that the arguments that led to the prediction of the various electromagnetic AB effects apply equally well to any other gauge-invariant quantum theory. In the standard model of particle physics, the strong and weak nuclear interactions are also described by gauge-invariant theories. So one may expect that particle-physics experimenters will be looking for new AB effects in new domains. Christine Aidala, CENPA Seminar, 2/1/18 22

42 Physical consequences of a gauge-invariant quantum theory: Aharonov-Bohm effect in QCD!! Deep-inelastic lepton-nucleon scattering: Final-state color exchange incoming electron scattering quark scattered electron scattered quark Quark-antiquark annihilation to leptons: Initial-state color exchange incoming proton scattering antiquark scattering quark proton remnant produced positron incoming proton proton remnant incoming proton proton remnant produced electron See e.g. Pijlman, hep-ph/ or Sivers, arxiv: Christine Aidala, CENPA Seminar, 2/1/18 23

43 Physical consequences of a gauge-invariant quantum theory: Aharonov-Bohm effect in QCD!! Deep-inelastic lepton-nucleon scattering: Final-state color exchange incoming electron incoming proton scattering quark proton remnant scattered electron Quark-antiquark annihilation to leptons: Initial-state color exchange incoming proton scattering antiquark scattering quark incoming proton proton remnant Simplicity scattered of these two processes: quark Abelian vs. non-abelian nature of the gauge group doesn t play a role. proton remnant BUT: In QCD expect additional, new effects See e.g. Pijlman, hep-ph/ due to specific non-abelian nature of the or Sivers, arxiv: gauge group gluon self-coupling produced positron produced electron Christine Aidala, CENPA Seminar, 2/1/18 23

44 QCD Aharonov-Bohm effect: Color entanglement 2010: T.C. Rogers and P. Mulders predict color entanglement in processes involving proton-proton production of QCD bound states if quark transverse momentum taken into account Quarks become correlated across the two colliding protons Consequence of QCD specifically as a non-abelian gauge theory! PRD 81, (2010) p p h + h X Color flow can t be described as flow in the two gluons separately. Requires presence of both. Christine Aidala, CENPA Seminar, 2/1/18 24

45 QCD Aharonov-Bohm effect: Color entanglement 2010: T.C. Rogers and P. Mulders predict color entanglement in processes involving proton-proton production of QCD bound states if quark transverse momentum taken into account Quarks become correlated across the two colliding protons Consequence of QCD specifically as a non-abelian gauge theory! Christine Aidala, CENPA Seminar, 2/1/18 PRD 81, (2010) p p h + h X Color flow can t be described as flow in the two gluons separately. Requires presence of both. Huge transverse spin asymmetries in p+p a color entanglement effect?? 24

46 Searching for evidence of color entanglement at RHIC Need observable sensitive to a nonperturbative momentum scale Nearly back-to-back particle production Need 2 initial QCD bound states color exchange between a scattering quark and remnant of other proton And at least 1 final QCD bound state exchange between scattered quark and either remnant In p+p collisions, measure out-ofplane momentum component in nearly back-to-back photon-hadron and hadron-hadron production Christine Aidala, CENPA Seminar, 2/1/18 25

47 Out-of-plane momentum component distributions Clear two-component distribution Gaussian near 0 nonperturbative transverse momentum Power-law at large p out kicks from hard (perturbative) gluon radiation Different colors different bins in hard interaction scale PRD95, (2017) Curves are fits to Gaussian and Kaplan functions, not calculations! Christine Aidala, CENPA Seminar, 2/1/18 26

48 Look at evolution of nonperturbative transverse momentum widths with hard scale (Q 2 ) Proof of factorization (i.e. no entanglement) for processes sensitive to nonperturbative transverse momentum directly predicts that nonperturbative transverse momentum widths increase as a function of the hard scattering energy scale Increased phase space for gluon radiation Confirmed experimentally in semi-inclusive deep-inelastic leptonnucleon scattering (left) and quark-antiquark annihilation to leptons (right) Christine Aidala, CENPA Seminar, 2/1/18 27

49 Look at evolution of nonperturbative transverse momentum widths with hard scale (Q 2 ) Proof of factorization (i.e. no entanglement) for processes sensitive to nonperturbative transverse momentum directly predicts that nonperturbative transverse momentum widths increase as a function of the hard scattering energy scale Increased phase space for gluon radiation Confirmed experimentally in deep-inelastic lepton-nucleon scattering (left) and quark-antiquark annihilation to leptons (right) Aidala, Field, Gamberg, Rogers, Phys. Rev. D89, (2014) Konychev + Nadolsky, Phys. Lett. B633, 710 (2006) Christine Aidala, CENPA Seminar, 2/1/18 27

50 Nonperturbative momentum widths may decrease in processes where entanglement predicted?? PHENIX Collab., PRD95, (2017) Measurements suggestive of quantum-correlated quarks across colliding protons? However, correlations among measured kinematic variables make results inconclusive Follow-up studies underway Discussions of other potential observables ongoing... Christine Aidala, CENPA Seminar, 2/1/18 28

51 A cyclical process Proliferation of observations and ideas Synthesis Christine Aidala, CENPA Seminar, 2/1/18 29

52 Summary Early years of rewarding new era of quantitative basic research in QCD! Gradually shifting to think about QCD systems in new ways, focusing on topics/ideas/concepts that have long been familiar to the world of condensed matter and AMO physics All sorts of correlations within systems and in their formation Quantum mechanical phase interference effects Quantum entangled systems Christine Aidala, CENPA Seminar, 2/1/18 30

53 Summary Early years of rewarding new era of quantitative basic research in QCD! Gradually shifting to think about QCD systems in new ways, focusing on topics/ideas/concepts that have long been familiar to the world of condensed matter and AMO physics All sorts of correlations within systems and in their formation Quantum mechanical phase interference effects Quantum entangled systems Christine Aidala, CENPA Seminar, 2/1/18 30

54 Summary Early years of rewarding new era of quantitative basic research in QCD! Gradually shifting to think about QCD systems in new ways, focusing on topics/ideas/concepts that have long been familiar to the world of condensed matter and AMO physics All sorts of correlations within systems and in their formation Quantum mechanical phase interference effects Quantum entangled systems Will be exciting to continue testing and exploring these ideas and phenomena in upcoming years... Christine Aidala, CENPA Seminar, 2/1/18 30

55 Afterword: QCD versus proton structure? A personal perspective Christine Aidala, CENPA Seminar, 2/1/18 31

56 We shall not cease from exploration And the end of all our exploring Will be to arrive where we started And know the place for the first time. T.S. Eliot Christine Aidala, CENPA Seminar, 2/1/18 32

57 Extra Christine Aidala, CENPA Seminar, 2/1/18 31

58 Advancing into the era of quantitative QCD: Theory has been forging ahead In perturbative QCD, since 1990s starting to consider detailed internal dynamics that parts with traditional parton model ways of looking at hadrons and perform phenomenological calculations using these new ideas/tools! E.g.: Various resummation techniques Non-linear evolution at small momentum fractions Spin-spin and spin-momentum correlations in QCD bound states Spatial distributions of partons in QCD bound states Nonperturbative methods: Lattice QCD less and less limited by computing resources since 2010 starting to perform calculations at the physical pion mass (after 36 years!). Plus recent new ideas on how to calculate previously intractable quantities. AdS/CFT gauge-string duality an exciting recent development as first fundamentally new handle to try to tackle QCD in decades! Christine Aidala, CENPA Seminar, 2/1/18 32

59 Effective field theories QCD exhibits different behavior at different scales effective field theories are useful approximations within these different regimes Color Glass Condensate high energies, high densities Soft-Collinear Effective Theory new insights into performing complicated perturbative calculations very quickly Chiral Effective Theory, Heavy Quark Effective Theory, Non-Relativistic QCD,... Many effective theories for nonperturbative QCD chiral symmetry breaking,... Christine Aidala, CENPA Seminar, 2/1/18 33

60 Parton distribution functions in perturbative QCD calculations of observables P 1 q(x 1 ) xp 1 1 Hard Scattering Process D q π 0 ( z) ŝ P 2 g(x 2 ) xp 2 2 σˆ qg qg X σ ( ) ( ) ( ) ( ) 0 0 qg qg π pp π X q x g x ˆ σ sˆ D ( z) 1 2 q High-energy processes have predictable rates given: Partonic hard scattering rates (calculable in pqcd) Parton distribution functions (experiment or lattice) Fragmentation functions (experiment or lattice) Universal nonperturbative factors Christine Aidala, CENPA Seminar, 2/1/18 34

61 Spin-spin and spin-momentum correlations in QCD bound states U = unpolarized L = longitudinally polarized T = transversely polarized N = nucleon q = quark Christine Aidala, CENPA Seminar, 2/1/18 35

62 Forward transverse single-spin asymmetries for neutral pions Christine Aidala, CENPA Seminar, 2/1/18 36

63 π π, K, p at 200 and 62.4 GeV 200 GeV 62.4 GeV Note different scales π K 200 GeV K- asymmetries underpredicted Pions suggest valence quark effect. Kaons and (anti)protons don t! K 62.4 GeV p 200 GeV Large antiproton asymmetry?? Unfortunately no 62.4 GeV measurement Christine Aidala, CENPA Seminar, 2/1/18 p 62.4 GeV PRL 101, (2008) 63

64 Partonic process contributions for direct photon production PHENIX data region Quark-gluon Compton scattering still dominates at NLO - PLB140, 87 (1984) PHENIX Collab., arxiv: , Submitted to PRD. Calculation by T. Kaufmann Christine Aidala, CENPA Seminar, 2/1/18 38

65 Two-particle correlation distributions show expected jet-like structure PRD95, (2017) Christine Aidala, CENPA Seminar, 2/1/18 39

66 PYTHIA p out distributions Christine Aidala, CENPA Seminar, 2/1/18 40

67 Christine Aidala, CENPA Seminar, 2/1/18 41

68 PYTHIA Drell-Yan Christine Aidala, CENPA Seminar, 2/1/18 42

69 Nonperturbative momentum measurements in Drell-Yan and Z production Christine Aidala, CENPA Seminar, 2/1/18 43

70 Other measurements showing decreasing nonperturbative momentum widths STAR and PHENIX Christine Aidala, CENPA Seminar, 2/1/18 44

71 Nuclear effects? Do stronger color fields lead to modified factorization breaking effects? p+au shows steepest decreasing slope for most peripheral events why?? Christine Aidala, CENPA Seminar, 2/1/18 45

72 Links to color coherence at Tevatron D0, CDF, CMS have all published evidence for color coherence effects CMS: EPJ C74, 2901 (2014) CDF: PRD50, 5562 (1994) D0: PLB414, 419 (1997) Few citations relatively little-known work thus far. Need to get different communities talking to explore detailed color effects more in upcoming years! and LHC? Christine Aidala, CENPA Seminar, 2/1/18 46

73 Magnetic and electric A-B effects; Type-I and Type-II A-B effects Physics Today, September 2009 Christine Aidala, CENPA Seminar, 2/1/18 73

74 Opportunities to see color-induced phases in QCD Slide from P. Mulders Figures by Kees Huyser Christine Aidala, CENPA Seminar, 2/1/18 48